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Two-Body Problem


The two-body problem is the n-body problem for two bodies of masses m_1,m_2>0 under mutual Newtonian gravitational attraction. Their center of mass moves with constant velocity, while their relative position vector r=r_1-r_2 satisfies

 r^..=-(G(m_1+m_2))/(||r||^3)r,

where G is the gravitational constant (Heggie 2006).

If the specific angular momentum h=r×r^. is nonzero, the motion lies in a plane perpendicular to h. In polar coordinates, with the angular origin chosen along the direction of closest approach,

 r(theta)=p/(1+ecostheta),

where p=||h||^2/[G(m_1+m_2)] and e>=0 is the eccentricity. The trajectory is an ellipse for e<1, a parabola for e=1, and a hyperbola for e>1. The case e=0 is a circle; zero angular momentum instead gives radial motion.

By Newton's shell theorem, the same exterior interaction applies to two nonoverlapping spherically symmetric bodies.


See also

Center of Mass, Conic Section, Eccentricity, n-Body Problem, Newton's Shell Theorem, Three-Body Problem

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References

Heggie, D. C. "Gravitational N-Body Problem (Classical)." In Encyclopedia of Mathematical Physics (Ed. J.-P. Françoise, G. L. Naber, and S. T. Tsou). Oxford, England: Elsevier, pp. 575-582, 2006. https://doi.org/10.1016/B0-12-512666-2/00003-1.

Cite this as:

Weisstein, Eric W. "Two-Body Problem." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/Two-BodyProblem.html

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